Nuclear matter distributions in the 6He and 8He nuclei from differential cross sections for small-angle proton elastic scattering at intermediate energy

2002 ◽  
Vol 712 (3-4) ◽  
pp. 269-299 ◽  
Author(s):  
G.D. Alkhazov ◽  
A.V. Dobrovolsky ◽  
P. Egelhof ◽  
H. Geissel ◽  
H. Irnich ◽  
...  
1979 ◽  
Vol 57 (3) ◽  
pp. 343-352 ◽  
Author(s):  
N. Ramanathan ◽  
T. J. Kennett ◽  
W. V. Prestwich

The differential cross sections for photon elastic scattering have been determined for targets of Cu, Cd, Ta, and Pb, at angles of 2.4, 3.5, 5.1., 6.0, 8.0, and 10.0° and incident energies of 244.7, 344.3, 443.9, 778.9, 964.0, 1085.8, 1112.0, 1274.2, and 1408.0 keV. The data indicate that presently calculated form factors may be too large, and suggest that intermediate bound states may influence the scattering amplitude.


1976 ◽  
Vol 113 (1) ◽  
pp. 1-33 ◽  
Author(s):  
E. Eisenhandler ◽  
W.R. Gibson ◽  
C. Hojvat ◽  
P.I.P. Kalmus ◽  
L.C.Y. Lee ◽  
...  

1987 ◽  
Vol 36 (7) ◽  
pp. 3077-3082 ◽  
Author(s):  
R. S. Gao ◽  
L. K. Johnson ◽  
D. E. Nitz ◽  
K. A. Smith ◽  
R. F. Stebbings

1973 ◽  
Vol 51 (20) ◽  
pp. 2197-2201 ◽  
Author(s):  
P. W. Martin ◽  
R. McFadden ◽  
B. L. White

The differential cross sections for 4.3 MeV neutrons elastically scattered from natural samples of U, Bi, and Pb have been measured at laboratory angles of 5, 10, and 15°. In the case of uranium, the data are consistent with calculations based on the nuclear optical model and known electromagnetic interactions. Less satisfactory agreement to the data is obtained in the cross section measurements for lead and bismuth.


1987 ◽  
Vol 35 (11) ◽  
pp. 4541-4547 ◽  
Author(s):  
D. E. Nitz ◽  
R. S. Gao ◽  
L. K. Johnson ◽  
K. A. Smith ◽  
R. F. Stebbings

2012 ◽  
Vol 27 (20) ◽  
pp. 1250113 ◽  
Author(s):  
O. V. SELYUGIN

Taking into account the different forms of the Coulomb-hadron interference phase and the possible spin-flip contribution the new analysis of the experimental data of the proton–antiproton elastic scattering at 3.8<pL<6.0 GeV/c and small momentum transfer is carried out. It is shown that the size of the spin-flip amplitude can be determined from the form of the differential cross-sections at small-t, and the deviation of ρ(s, t) obtained from the examined experimental data of the [Formula: see text] scattering from the analysis1, based on the dispersion relations, is conserved in all examined assumptions. The analysis of the proton–proton elastic scattering at 9<pL<70 GeV/c also shows the impact of the examined effects on the form of the differential cross-sections.


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